Jump to
S2C1
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -77.231277 |
| Energy at 298.15K | -77.230851 |
| Nuclear repulsion energy | 23.709865 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3PW91/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3136 |
3026 |
47.46 |
|
|
|
| 2 |
A1 |
1720 |
1659 |
87.03 |
|
|
|
| 3 |
A1 |
1174 |
1133 |
28.64 |
|
|
|
| 4 |
B1 |
725 |
699 |
80.79 |
|
|
|
| 5 |
B2 |
3231 |
3118 |
28.24 |
|
|
|
| 6 |
B2 |
256 |
247 |
3.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5120.4 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 4941.1 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3PW91/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.480 |
| C2 |
0.000 |
0.000 |
0.825 |
| H3 |
0.000 |
0.947 |
-1.034 |
| H4 |
0.000 |
-0.947 |
-1.034 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3049 | 1.0973 | 1.0973 |
C2 | 1.3049 | | 2.0860 | 2.0860 | H3 | 1.0973 | 2.0860 | | 1.8950 | H4 | 1.0973 | 2.0860 | 1.8950 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C2 |
C1 |
H3 |
120.294 |
|
C2 |
C1 |
H4 |
120.294 |
| H3 |
C1 |
H4 |
119.412 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.127 |
|
|
|
| 2 |
C |
-0.096 |
|
|
|
| 3 |
H |
0.111 |
|
|
|
| 4 |
H |
0.111 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-2.380 |
2.380 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.900 |
0.000 |
0.000 |
| y |
0.000 |
-10.133 |
0.000 |
| z |
0.000 |
0.000 |
-13.982 |
|
| Traceless |
| | x | y | z |
| x |
-1.842 |
0.000 |
0.000 |
| y |
0.000 |
3.808 |
0.000 |
| z |
0.000 |
0.000 |
-1.966 |
|
| Polar |
| 3z2-r2 | -3.932 |
| x2-y2 | -3.767 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.668 |
0.000 |
0.000 |
| y |
0.000 |
2.611 |
0.000 |
| z |
0.000 |
0.000 |
4.016 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |
Jump to
S1C1
Energy calculated at B3PW91/cc-pVDZ
| | hartrees |
| Energy at 0K | -77.165322 |
| Energy at 298.15K | -77.165378 |
| HF Energy | -77.165322 |
| Nuclear repulsion energy | 23.480902 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3PW91/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3047 |
2941 |
3.03 |
|
|
|
| 2 |
A1 |
1604 |
1548 |
4.79 |
|
|
|
| 3 |
A1 |
1366 |
1318 |
2.77 |
|
|
|
| 4 |
B1 |
766 |
739 |
8.32 |
|
|
|
| 5 |
B2 |
3133 |
3023 |
3.72 |
|
|
|
| 6 |
B2 |
973 |
939 |
3.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5444.8 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 5254.2 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3PW91/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-0.485 |
| C2 |
0.000 |
0.000 |
0.836 |
| H3 |
0.000 |
0.943 |
-1.054 |
| H4 |
0.000 |
-0.943 |
-1.054 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
H3 |
H4 |
| C1 | | 1.3204 | 1.1015 | 1.1015 |
C2 | 1.3204 | | 2.1117 | 2.1117 | H3 | 1.1015 | 2.1117 | | 1.8863 | H4 | 1.1015 | 2.1117 | 1.8863 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.050 |
|
|
|
| 2 |
C |
-0.108 |
|
|
|
| 3 |
H |
0.079 |
|
|
|
| 4 |
H |
0.079 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-0.589 |
0.589 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.626 |
0.000 |
0.000 |
| y |
0.000 |
-11.863 |
0.000 |
| z |
0.000 |
0.000 |
-11.068 |
|
| Traceless |
| | x | y | z |
| x |
-2.161 |
0.000 |
0.000 |
| y |
0.000 |
0.484 |
0.000 |
| z |
0.000 |
0.000 |
1.677 |
|
| Polar |
| 3z2-r2 | 3.353 |
| x2-y2 | -1.764 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.876 |
0.000 |
0.000 |
| y |
0.000 |
2.286 |
0.000 |
| z |
0.000 |
0.000 |
4.121 |
<r2> (average value of r
2) Å
2
| <r2> |
17.210 |
| (<r2>)1/2 |
4.148 |